CN100343924C - Method for measuring the relative extent of burnout of combustion elements in a pebble-bed high-temperature reactor (HTR) and a corresponding device - Google Patents
Method for measuring the relative extent of burnout of combustion elements in a pebble-bed high-temperature reactor (HTR) and a corresponding device Download PDFInfo
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- 238000002485 combustion reaction Methods 0.000 title claims abstract description 143
- 238000000034 method Methods 0.000 title claims abstract description 55
- 238000005259 measurement Methods 0.000 claims description 77
- 230000004992 fission Effects 0.000 claims description 33
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- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
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- G21C17/00—Monitoring; Testing ; Maintaining
- G21C17/06—Devices or arrangements for monitoring or testing fuel or fuel elements outside the reactor core, e.g. for burn-up, for contamination
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- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21C—NUCLEAR REACTORS
- G21C1/00—Reactor types
- G21C1/04—Thermal reactors ; Epithermal reactors
- G21C1/06—Heterogeneous reactors, i.e. in which fuel and moderator are separated
- G21C1/07—Pebble-bed reactors; Reactors with granular fuel
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- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21C—NUCLEAR REACTORS
- G21C17/00—Monitoring; Testing ; Maintaining
- G21C17/06—Devices or arrangements for monitoring or testing fuel or fuel elements outside the reactor core, e.g. for burn-up, for contamination
- G21C17/066—Control of spherical elements
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- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21C—NUCLEAR REACTORS
- G21C17/00—Monitoring; Testing ; Maintaining
- G21C17/10—Structural combination of fuel element, control rod, reactor core, or moderator structure with sensitive instruments, e.g. for measuring radioactivity, strain
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
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- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E30/00—Energy generation of nuclear origin
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Abstract
Previous methods for measuring the burn-out of a combustion element from a pebble-bed high-temperature reactor, in particular with high circulation rates, have as a rule an error margin of up to 10 %. The inventive method for measuring burn-out is extremely rapid, but nevertheless highly accurate, with an error margin of only 1-2 %. The method comprises the following steps: a) a combustion element is removed from the reactor and transferred to a measuring position; b) the combustion element is subjected to a thermal neutron flux; c) a first detector determines the gamma radiation emitted by the combustion element; d) if the measured value exceeds a previously defined first threshold value, the combustion element is fed directly to the reactor, but if the measured value falls below the threshold value, the combustion element is subjected to steps e to f; e) a second detector determines the high-energy gamma radiation above 1 MeV emitted from the combustion element; f) if the measured value exceeds a previously defined second threshold, the combustion element is fed to the reactor, but if the measured value falls below said threshold value, the combustion element is evacuated from the combustion element circuit.
Description
The present invention relates to a method of measuring combustion elements, and in particular to a method of measuring combustion element burnout which can be used to determine pebble bed High Temperature Reactor (HTR) combustion element burnout.
When operating a packed ball bed HTR (e.g., AVR or THTR) with multiple outlets (mehrfachdurchauf), a certain proportion of the circulating combustion elements (BE) must BE removed from the circuit in order to make room for the addition of new combustion elements. In view of good nuclear fuel economy, it is of course possible to remove the most burning elements. For this purpose, each individual cycle combustion element is tested. Physical quantities representing the degree of burn-out are measured here. The homogeneity of the burn-out value is not necessary here for measuring accuracy, but a large measuring effect and good reproducibility of the measured values are important. This value is used to determine whether the combustion elements are returned to the reactor core, and if necessary which core zone they are returned to, or whether they are removed.
A fission process is performed within the reactor core, wherein fission products are produced from the nuclear fuel in the combustion element. If a single combustion element of the cycle enters the bulb lead-out (Kugelabzugrohr) from the reactor core, then the fission process is then stopped. The fission products in the combustion element are radioactive and emit gamma rays. For different combustion elements, the total gamma rays radiated by the combustion element and measured are correlated with their burnout under otherwise identical conditions, for example after the same time period after exiting the combustion element from the reactor core.
Heretofore, different measuring methods for determining the degree of burning of the spherical combustion element have been used.
Cycle rate of about 500 days for AVR (professional workgroup test reactor) based on relatively small combustion elements, Cs in combustion elements137The gamma spectroscopy measurement of (a) can be performed with a semiconductor detector cooled by liquid nitrogen. This measurement is less expensive and provides a measurement accuracy in the range of ± 2% at high burn-out BE (combustion element) within an acceptable measurement time of 20 to 40 seconds.
For modern modular pebble-bed nuclear power reactors, such as siemens 'HTR modules or south africa's PBMR, which are much higher than the AVR cycle speed (about 4000 combustion elements per day) and the combustion elements have a relatively short decay time in the bulb lead-out (about two days), the direct transfer of the AVR measurement method is based only on the availability of the more available onesSmall measurement times cannot be transferred to such reactors. Shorter measurement times must lead to greater measurement errors. Of course, of greater environmental interest, Cs was analyzed due to the combustion element having only a small decay time137The lines are clearly not accurate. High radioactivity of transiently existing fission products on Cs137The gamma measurement of (2) has a strong influence because typical Cs are analyzed137The 662keV line of (1) is clearly affected by the adjacent line (Nachballine). Herein, one aspect relates to Nb97Strong 658keV line (effective half-life 16.8 hours), Ba140Weak 661keV line (half-life 12.8 days) and I132Strong 668keV line (effective half-life 76.3 hours). Thus, measured Cs137The corresponding correction of the signal in question usually requires elaborate measuring techniques. Rapid cycling combined with a short bulb and short residence time in the bulb thus results in a strong adverse effect on the reproducibility of the Cs measurements. For this reason, there is no real specific experience with the reactor. The assessment of the achievable accuracy is very similar for the person skilled in the art. It is envisaged, according to common knowledge, that the mean error is not less than 10% for high burn-out combustion elements.
Therefore, a corresponding group of experts selectively suggests simple measurement of the total gamma-activity of the combustion elements for modern modular pebble-bed nuclear power reactors.
The gamma activity of the radioactive combustion elements is mainly in the reactor core, but the fission products present for a short time when the decay time is not too long dominate after the combustion elements exit from the core. The contribution of fission products existing for a long time to the radiation intensity is practically negligible. The lower degree of burn-out of the combustion elements in the reactor core, and therefore also before their exit from the core, generates higher power than the high degree of burn-out of the combustion elements, and thus has a higher (temporary) gamma emission. The measured effects, i.e. the gamma radiation of low and high burn-up combustion elements, differ greatly. (the gamma emission for a low burn-out combustion element, shown by the longer average one month decay time of the AVR combustion element, is always 3 to 4 times higher than for a high burn-out combustion element). This method, although not very precise, is simple and fast (measurement time of about one second).
Total gamma radioactivity and Cs137The combination of radiation measurements of (a) is considered to be prior art. A simple gamma measurement (for example 1 second) is carried out here for all combustion elements. Only when a combustion element with high burnout is identified, the combustion element has a gamma emission value below a previously defined threshold value, delayed by, for example, Cs extending in parallel137Measurement of (2) (about 10 seconds). Only assay Cs137The target of the combustion element is determined, returned or removed.
In this combined approach, which regularly allows longer measurement times for Cs measurements, larger average errors are taken into account for high burn-up combustion elements. Those skilled in the art recognize that an accuracy of + -4% to + -20% is sufficient.
The object of the invention is to provide a method for measuring a spherical burner element, by means of which the degree of burning of the burner element can be determined for a short decay time of the burner element and during short measurement times during the circulation of a pebble bed reactor.
The object of the invention is also to provide a corresponding device for carrying out the above-described measuring method.
The object of the invention is achieved by a method for determining the burn-out of a spherical combustion element and a device for carrying out the method.
The present invention does not describe a method for determining the absolute value of the burning loss of a spherical combustion element (e.g. the cracking rate of the initial metal atoms in% FIMA). The present invention also does not measure the burn-out of low-burn-out combustion elements. The combustion element is identified by a simple gamma measurement due to its significantly higher gamma activity.
The novel method according to the invention provides in particular for the combustion elements classified by simple gamma measurement as highly burnt, to be further specified with regard to the degree of burning, in particular with regard to the removal possibility.
The subject of the invention is a method for measuring the degree of burnout of a spherical combustion element, which is similar to the method previously described as a combined method. A brief, simple gamma measurement is made by the burner element removed from the reactor core. The measured combustion elements are classified as low-burn combustion elements or high-burn combustion elements by a first threshold value of the gamma activity determined beforehand. Combustion elements identified as having higher burn-out were subjected to another measurement. This second measurement is based on the assumption that the more fission of the burner element occurs in the burner element when excited with thermal neutrons, the less burnout. During the fission process, strong gamma rays are emitted spontaneously. The intensity of the intense gamma rays, particularly in the energy region above 2MeV, can therefore likewise be regarded as a measure for the burning of the combustion element.
The method for measurement was performed as follows. The combustion element spheres are removed from the reactor core, for example, in the circulation range and transferred to a measuring point. Where the burner element sphere is subjected to a stream of thermal neutrons which lead to nuclear fission in the burner element. In addition to the gamma-radioactivity of the already present fission products, radiation of so-called spontaneous emission rays and radiation in the form of intense gamma rays also results during nuclear fission. The intense gamma rays contain on average more energy than the gamma rays of the fission products.
The total gamma-radioactivity of the combustion elements is measured in a first measurement step with a first detector. The measurement is usually fast (about 1 second), but not very accurate. This measurement is used only to make a first assessment of the burning of the combustion element examined. For a given reactor, the frequency of the combustion elements with the determined total gamma activity occurs according to a statistical frequency distribution. This also depends, among other things, on at which moment the combustion element is measured after removal from the reactor core. Highly burned combustion elements also have only few fission products, so that the gamma rays radiated by the products are of little activity. If an upper limit for the gamma rays is specified above which the measured combustion element is always returned to the reactor core, a preselection of the combustion element can be carried out, wherein a further measurement is awaited. The threshold value may determine the frequency distribution accordingly. The limit value is determined, for example, such that at most 20% of all measured combustion elements have a measured radioactivity below the limit value. Only at this 20% is the second measurement to be taken advantageously in parallel awaited.
A second measurement step of the method according to the invention consists in determining only the intense gamma rays of the combustion element with a corresponding second detector. The method according to the invention advantageously uses an existing reactor as a neutron source for generating nuclear fission in the combustion element. Detectors suitable for this must in particular measure radiation of a very high energy, preferably above 2 Mev. A measure for this energy selection, for example a NaI scintillation counter, is sufficient. The second detector should also be able to handle at least gamma total pulse rates of at least more than 107/s, in particular more than 108/s.
Due to the short decay time of the fission products within the burning element, the gamma-activity of the fission products is generally significantly greater than the gamma-activity of the fission. In order that the effective signal of the intense gamma rays is not excessively superposed by the gamma activity of the fission products of the low-energy combustion element, several solutions can be implemented individually or in combination.
1. It is advantageous to use a detector for the second measurement step, which can handle very high pulse rates, i.e. with very good time resolution, and therefore with only small errors in a very short measurement time.
2. Furthermore, by providing a shield between the detector and the combustion element, which shield is used in particular for a high-pass filter of the energy and leads to a reduction of low-energy gamma rays impinging on the second detector, the ratio of more (intense) and less energy gamma rays is improved and benefits are obtained for intense rays. Such shielding may be produced, for example, by lead filters.
3. For a particularly accurate second measurement, the second detector should advantageously be arranged such that its optimum operating range lies on the radiation values emitted by the (higher burn-out) combustion element that is being considered. This also has the disadvantage that the radiation value of the low-burn combustion element is significantly higher than the optimum operating region of the second detector. To avoid possible damage of the second detector, various measures can be taken. In particular, another suitable shielding can be used to prevent overloading of the second detector when measuring low-burn combustion elements. Or the second detector is switched off when measuring low-burn combustion elements, which is a particularly simple implementation for measurements 1 and 2 which are carried out in succession.
4. The number of induced nuclear fissions in the combustion element increases with increasing neutron flux (measurement flow). In order to achieve as high a thermal neutron flux as possible at the measuring point of the combustion element, a true reactor is therefore suitable as a neutron source. In principle other neutron sources are also suitable.
5. The measuring location is advantageously surrounded by water. The reactivity of the subcritical measuring device is thereby increased, and as many neutrons released in fission as possible are used for further fission. The combustion elements to be measured themselves influence the reactivity of the device with their fissile material. Resulting in an enhanced measurement effect.
6. In order to increase the accuracy of the second measurement, optionally a plurality of second detectors can be provided, which add the determined counting results in parallel.
7. Furthermore, it is provided that a plurality of combustion elements are measured simultaneously in parallel at a plurality of measurement positions. Without changing the number of cyclic beats, each measurement can be used for multiple measurement times, which regularly and positively affects the measurement accuracy.
8. In principle, it is also advantageous to extend the time between the removal of the combustion element from the reactor core and its measurement (intermediate time), since the gamma rays of the fission products decrease over time in accordance with their disintegration, but the gamma rays of the induced fission are not affected. Which has the disadvantage of causing expensive structural changes or disadvantageous reactor operation.
The method according to the invention can be expressed accurately (error is only about 1-2%) simply by the degree of burning of the combustion element. The method is therefore particularly suitable for determining whether the circulating combustion elements in a high-temperature reactor (HTR) are to be removed from the reactor cycle or returned to the reactor core. The method herein advantageously supports the determination as follows:
a) the combustion element is removed from the reactor and transported to a measuring location,
b) the combustion element is subjected to a flow of thermal neutrons,
c) the first detector measures gamma rays emitted by the combustion element,
d) the combustion element is directly fed back to the reactor when a first predetermined limit value is exceeded, and steps e to f are carried out when the limit value is undershot,
e) the second detector measures high-energy gamma rays of 1MeV or more emitted from the combustion element,
f) when a second predetermined threshold value is exceeded, the combustion elements are returned to the reactor, and when the threshold value is undershot, the combustion elements are removed from the combustion element circuit.
The subject matter of the invention is described in detail below with reference to the examples and the drawings, without thereby restricting the subject matter of the invention.
The figure shows a horizontal section of an embodiment of an apparatus for carrying out the method according to the invention. Wherein,
1 reactor, outside of the biological housing
2 thermal column with thermionic flow (graphite)
3 ball catheter
4 water tank
5 biological screening
6 combustion element in measuring position
7 plug for replacing detector
8 second gamma detector with high time resolution and selected energy
9 connecting cable for pulse processing
10 Detector Shielding and energy Filter, e.g. made of lead
11 first gamma detector
12 circulation device with means for fixing the combustion element at the measuring point
Component (schematically shown)
The method according to the invention is carried out in an apparatus as follows:
the combustion element 6 to be measured, which is removed from the reactor core, is placed in a defined measuring position 12, in which it is exposed to the thermal neutron flow 2. Nuclear fission occurs in the burning element in connection with burning loss or fissile material also contained in the burning element 6, the strength of which is obtained by means of test techniques. The measured value is here an intense high-energy gamma ray which is emitted by the fission products produced during the measurement (spontaneous emission) following the fission process. In this case, the energy of the intense gamma rays is higher on average than the gamma rays emitted by the fission products in the combustion element. The energy-selective gamma measuring instrument thus measures intense, more energetic gamma rays. A suitable detection system is, for example, a scintillation counter 8 with a high resolution in terms of time, for which purpose its energy resolution is sufficient.
The small, higher energy fraction of the gamma rays of the fission products in the combustion element, which fraction falls in the range of the intense gamma rays to be measured, can be measured together without a great influence on the measurement accuracy, since the total gamma rays of the combustion element to be measured are likewise dependent on the burnout, that is to say in the same way. The higher the burn-out, the lower the fissile content, the lower the fission activity during the measurement, the lower the intense gamma rays and the lower the total activity of the burner element. (the solution for simply measuring the total gamma-ray of the combustion element as a measuring method has been described above.)
Two features that have been implemented so far characterize the principles of the new method. The main difficulty with this method is that the gamma radioactivity of BE is very high (interfering signals) due to its short decay time (typically 2 days), compared to which the intense gamma ray, which is an effective signal, is completely in the background. The following further features of the method are also important in order to achieve the desired accuracy, i.e. to accumulate a statistically sufficiently large number of useful signals in a short measurement time.
A gamma measuring instrument 8 (second detector) that handles very high pulse rates can be used, thus achieving very high temporal resolution. The shielding 10 between the measuring instrument 8 and the combustion element 6 to be measured is designed in such a way that the measuring instrument is already operating within its maximum number of possibilities for combustion elements with high burn-out, i.e. combustion elements which emit weaker radiation. Combustion elements which emit more intense radiation and which have not been sufficiently burnt can no longer be detected by the second detector 8. This makes sense for the combined method described by means of a simple gamma measurement with the first detector 11.
The necessary shielding 10 between the combustion element 6 and the measuring instrument 8 (second detector) is embodied in the form of lead in order to achieve the effect of an energy filter as large as possible (preferably transparent to intense gamma radiation).
The consumption of fissile material for the measurement can be completely ignored even at very high neutron flows (measurement flows) due to the short measurement time. Thus, the measurement flow can be as high as possible to achieve good accuracy of the method. An external neutron source is not used and the reactor core itself is advantageously used as the neutron supplier. For this purpose, the reactor is similar to a research reactor, for example Dido from the research center of julich ltd, in that the "hot column" 2, i.e. the radially extending, continuous graphite connection between the side reactor and the outside of the biological shield, which is disconnected as far as possible only from the reactor vessel, is kept as high as possible at the level of the middle of the reactor core. There is a measurement site 12 immediately in front of the outer end face of the graphite. The measuring location 12 is also advantageously surrounded by water 4. This increases the reactivity of the subcritical measuring device and makes the neutrons released in fission available as far as possible for further fission. The combustion element to be measured influences the reactivity of the device itself with its fissile content. This results in an enhancement of the measuring effect.
In relation to the actual implementation, the measuring point 12 is advantageously arranged in a component of the spherical charging device 3, in which a ball is always present. For this purpose, a ball feed preselector is provided in particular, by means of which the desired target of the measuring ball (on the ball bed or the ball removed) is controlled. The arrangement of the feed preselector at the mid-height of the reactor core (before the "hot column") has the further advantage that the long, high feed path from the lower end region of the ball extraction tube to the upper reversal point of the feed line leading to the ball bed is divided into two partial sections, so that a single pneumatic ball feed process is sufficient with a small feed pressure and feed quantity.
The biological shield 5 and the further gamma detector 11, which enclose the measuring device, belong to the entire measuring device. The detector is arranged to operate at a high count rate at the measurement location 12 for low burn-out combustion elements, for example after nuclear flow (coredurchuuf). The gamma radioactivity of all the combustion elements (and other spheres) taken from the measurement site is measured by this detector 11 for the combined method mentioned above. If the measurement result of the detector 11 is greater than a certain limit value, the measured combustion element is not yet sufficiently burnt and is returned to the reactor core without having to wait for a second measurement. When this threshold value is undershot, the measurement of the combustion element also waits for the detector 8, after which the ball target is first determined (removed or returned). This is again done by comparing the measurement result with another limit value. When the value is below the threshold value, the combustion element is removed.
These two limit values can be derived from a frequency distribution of a large number (e.g. 300) of measurements of the combustion element measured previously. This number is equal to the area under the distribution curve. For determining the limit value, a value is sought on the measurement value scale, which divides the distribution area in a predetermined numerical relationship. If, for example, it is provided that 20% of all measured combustion elements should also be measured with the second detector element 8, the distribution area of the measurement results of the first detector 11 is divided by the ratio 2: 8. 20% of all measurements are below the first threshold value. If it is assumed, moreover, that the reactor is operated in a 1: 10 operating mode, i.e. with each fresh combustion element added in a cycle and therefore-always a long-term average value-1 combustion element must be taken out of 10 cycles of combustion elements, the fraction taken out being 10%, a value is sought in the frequency distribution of the measurement results of the second detector 8 which integrates the distribution surface into two equally large halves. The combustion element is removed, the measurement falling below this second limit value. The withdrawn fraction was 10%, so that a 1: 10 mode of operation was required. The frequency distribution and thus the threshold value calculation may be accumulated after each combustion element measurement. When the reactor power changes, the measurement result is multiplied by the new ratio of the previous power before it is processed.
If the second detector 10 is damaged by oversaturation of the gamma rays in the on state, advantageously the two measurements are not started in parallel, but only the gamma rays are measured first with the first detector 11. The operating voltage of the second detector 8 is switched on, for example, only if the measurement result falls below a first threshold value.
It can be seen that the measuring device does not always have to be arranged in front of the bio-cap 1 as shown in the figure, but it can also be arranged in a recess of the bio-cap. The "heat column" is thereby shortened, while the measurement flow 2 is larger. The measurement may even be performed directly on the outside of the reactor pressure vessel. The second detector 8 is of course strongly exposed to gamma radiation from the reactor core. A high measurement flow 2 is of great interest for the accuracy of the method, in which case a constant gamma background can be tolerated for the measurement, as long as it is not essential.
Claims (19)
1. A method for measuring a relative value of burn-out of a combustion element, having the steps of:
a) a combustion element (6) is removed from the reactor and fed to a measuring station (12),
b) the combustion element (6) is subjected to a neutron flow (2) so as to produce nuclear fission therein,
c) a first detector (11) measures all gamma rays emitted by the combustion element,
d) if a first predetermined threshold value is exceeded, the combustion element is fed back to the reactor, if the first threshold value is undershot, steps e) to f) are then carried out for the combustion element,
e) a second detector (8) measures high energy gamma rays emitted by the combustion element above 1MeV,
f) when a second predetermined threshold value is exceeded, the combustion elements are fed back to the reactor, and when the second threshold value is undershot, the combustion elements are removed from the combustion element circuit.
2. The method according to claim 1, wherein the second detector (8) measures high energy gamma rays above 2MeV emitted by the combustion element.
3. The method according to claim 1 or 2, wherein use is made of a composition having one of at least 107A second detector (8) of counting rate/sec.
4. Method according to claim 1 or 2, wherein a scintillation counter is used as the second detector (8).
5. Method according to claim 1 or 2, wherein a shield is provided between the measurement location (12) and the second detector (8).
6. The method according to claim 5, wherein a lead filter is provided as the shield between the measurement location (12) and the second detector (8).
7. The method according to claim 1 or 2, wherein the first detector (11) measures the gamma-rays of the combustion element (6) in less than 2 seconds.
8. The method according to claim 1 or 2, wherein the second detector (8) measures the gamma-rays of the combustion element (6) in less than 30 seconds.
9. Method according to claim 1 or 2, wherein the combustion element (6) is surrounded by water at the measuring location.
10. A method according to claim 1 or 2, wherein a first threshold value of the first γ measurement is determined, below which a reactor mode-adapted contribution of the combustion element is below.
11. A method according to claim 1 or 2, wherein a first threshold value for the first γ measurement is determined such that at most 20% of the combustion elements are below the first threshold value for a 1: 10 mode of operation of the reactor, wherein a 1: 10 mode of operation of the reactor means that each fresh combustion element added is cycled and therefore 1 combustion element must be removed from 10 cycled combustion elements.
12. A method according to claim 1 or 2, wherein a second threshold value of the second measurement is determined below which a proportion of all measured combustion elements that is adapted to the reactor operating mode is below.
13. A method according to claim 1 or 2, wherein a second threshold value for the second measurement is determined such that at most 15% of all measured combustion elements are below the second threshold value for a 1: 10 reactor mode of operation, wherein a 1: 10 reactor mode of operation means that each fresh combustion element added is cycled and therefore 1 combustion element must be removed from 10 cycled combustion elements.
14. Apparatus for carrying out the method according to any one of claims 1 to 13, having:
a) a neutron source which generates a thermal neutron flow (2),
b) for fixing a measuring position (12) of a combustion element to be measured, the combustion element being subjected to the thermal neutron flow,
c) a first detector (11) capable of measuring all gamma rays emitted by the combustion element (6),
d) a second detector (8) capable of measuring high energy gamma rays emitted by the combustion element above 1 MeV.
15. The device according to claim 14, wherein the device has a shield (10) between the measuring location (12) and the second detector (8).
16. Device according to claim 15, wherein the device has a lead filter as the shield (10).
17. The device according to claim 14, wherein the device has a scintillation counter as the second detector (8).
18. The apparatus according to claim 14, wherein the second detector (8) has at least 107Count rate per second.
19. The device according to claim 14, wherein the measuring location (12) is at least partially surrounded by water.
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DE10306648.9 | 2003-02-18 | ||
| DE10306648A DE10306648B3 (en) | 2003-02-18 | 2003-02-18 | Nuclear fuel element burn-up is measured by removing element from reactor, placing it in measurement position, exposing it to neutron flux, and measuring emitted gamma radiation |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN1751362A CN1751362A (en) | 2006-03-22 |
| CN100343924C true CN100343924C (en) | 2007-10-17 |
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CNB2004800045473A Expired - Fee Related CN100343924C (en) | 2003-02-18 | 2004-01-15 | Method for measuring the relative extent of burnout of combustion elements in a pebble-bed high-temperature reactor (HTR) and a corresponding device |
Country Status (9)
| Country | Link |
|---|---|
| US (1) | US7349517B2 (en) |
| EP (1) | EP1595264B1 (en) |
| JP (1) | JP4607858B2 (en) |
| KR (1) | KR20050100692A (en) |
| CN (1) | CN100343924C (en) |
| AT (1) | ATE333700T1 (en) |
| DE (2) | DE10306648B3 (en) |
| WO (1) | WO2004075205A2 (en) |
| ZA (1) | ZA200507542B (en) |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE10306648B3 (en) * | 2003-02-18 | 2004-07-01 | Forschungszentrum Jülich GmbH | Nuclear fuel element burn-up is measured by removing element from reactor, placing it in measurement position, exposing it to neutron flux, and measuring emitted gamma radiation |
| EP1953571B1 (en) * | 2007-02-05 | 2015-06-03 | Services Pétroliers Schlumberger | Nuclear tool used in a borehole to determine a property of the formation |
| US8861270B2 (en) * | 2013-03-11 | 2014-10-14 | Microsoft Corporation | Approximate multi-level cell memory operations |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3398280A (en) * | 1965-12-14 | 1968-08-20 | Atomic Energy Commission Usa | Method and apparatus for determining cooling age of nuclear reactor fuel |
| US3786256A (en) * | 1971-11-18 | 1974-01-15 | Nat Nuclear Corp | Method and apparatus for nuclear fuel assay with a neutron source and coincident fission neutron detectors |
| CN1051397C (en) * | 1992-06-22 | 2000-04-12 | 西屋电气公司 | Fixed incore detector |
Family Cites Families (17)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3388254A (en) * | 1966-09-07 | 1968-06-11 | Atomic Energy Commission Usa | Method for determining the amount of cesium-137 in irradiated nuclear fuel |
| DE1912982A1 (en) * | 1969-03-14 | 1970-10-01 | Interatom | Device for the nondestructive and separate determination of the concentrations of fissile substances in a test body |
| US3796875A (en) * | 1971-08-18 | 1974-03-12 | Kernforschung Gmbh Ges Fuer | Method and apparatus for the non-destructive analysis of nuclear fuels |
| DE2213238C3 (en) * | 1972-03-18 | 1979-08-23 | Kernforschungsanlage Juelich Gmbh, 5170 Juelich | Process for distinguishing and rejecting spherical fuel elements from high temperature nuclear reactors |
| US4515749A (en) | 1981-08-24 | 1985-05-07 | General Electric Company | Subcriticality measurement apparatus and method |
| US4881247A (en) * | 1982-03-25 | 1989-11-14 | Westinghouse Electric Corp. | Measuring nuclear fuel burnup |
| US4493810A (en) * | 1982-09-07 | 1985-01-15 | The United States Of America As Represented By The United States Department Of Energy | Method and apparatus for measuring reactivity of fissile material |
| US4510117A (en) * | 1983-02-10 | 1985-04-09 | The United States Of America As Represented By The United States Department Of Energy | Apparatus for in situ determination of burnup, cooling time and fissile content of an irradiated nuclear fuel assembly in a fuel storage pond |
| JPS6197594A (en) * | 1984-10-19 | 1986-05-16 | 株式会社東芝 | Nondestructive measurement method of spent fuel aggregate and device thereof |
| US4902467A (en) * | 1988-08-31 | 1990-02-20 | General Electric Company | Non-destructive testing of nuclear fuel rods |
| JP3522842B2 (en) * | 1993-09-29 | 2004-04-26 | 株式会社東芝 | Measuring device |
| JPH0882692A (en) * | 1994-09-12 | 1996-03-26 | Toshiba Corp | Burnup measuring device |
| JP3544065B2 (en) * | 1996-07-18 | 2004-07-21 | 株式会社東芝 | Simple burnup monitor |
| EP0837343A1 (en) * | 1996-10-15 | 1998-04-22 | European Atomic Energy Community (Euratom) | A monitor for measuring both the gamma spectrum and neutrons emitted by spent nuclear fuel |
| JP2000221293A (en) * | 1999-01-29 | 2000-08-11 | Toshiba Corp | Device and method for measuring burnup of fuel for nuclear reactor |
| DE19941719C2 (en) * | 1999-09-02 | 2003-12-04 | Forschungszentrum Juelich Gmbh | Process for removing spent fuel from a high temperature pebble bed reactor |
| DE10306648B3 (en) * | 2003-02-18 | 2004-07-01 | Forschungszentrum Jülich GmbH | Nuclear fuel element burn-up is measured by removing element from reactor, placing it in measurement position, exposing it to neutron flux, and measuring emitted gamma radiation |
-
2003
- 2003-02-18 DE DE10306648A patent/DE10306648B3/en not_active Withdrawn - After Issue
-
2004
- 2004-01-15 DE DE502004000989T patent/DE502004000989D1/en not_active Expired - Lifetime
- 2004-01-15 JP JP2006501460A patent/JP4607858B2/en not_active Expired - Lifetime
- 2004-01-15 CN CNB2004800045473A patent/CN100343924C/en not_active Expired - Fee Related
- 2004-01-15 AT AT04702283T patent/ATE333700T1/en not_active IP Right Cessation
- 2004-01-15 US US10/546,086 patent/US7349517B2/en not_active Expired - Fee Related
- 2004-01-15 EP EP04702283A patent/EP1595264B1/en not_active Expired - Lifetime
- 2004-01-15 WO PCT/DE2004/000037 patent/WO2004075205A2/en active IP Right Grant
- 2004-01-15 KR KR1020057015211A patent/KR20050100692A/en not_active Application Discontinuation
-
2005
- 2005-09-16 ZA ZA200507542A patent/ZA200507542B/en unknown
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3398280A (en) * | 1965-12-14 | 1968-08-20 | Atomic Energy Commission Usa | Method and apparatus for determining cooling age of nuclear reactor fuel |
| US3786256A (en) * | 1971-11-18 | 1974-01-15 | Nat Nuclear Corp | Method and apparatus for nuclear fuel assay with a neutron source and coincident fission neutron detectors |
| CN1051397C (en) * | 1992-06-22 | 2000-04-12 | 西屋电气公司 | Fixed incore detector |
Also Published As
| Publication number | Publication date |
|---|---|
| WO2004075205A3 (en) | 2004-10-21 |
| CN1751362A (en) | 2006-03-22 |
| EP1595264B1 (en) | 2006-07-19 |
| WO2004075205A2 (en) | 2004-09-02 |
| ATE333700T1 (en) | 2006-08-15 |
| ZA200507542B (en) | 2007-02-28 |
| DE10306648B3 (en) | 2004-07-01 |
| JP2006518036A (en) | 2006-08-03 |
| DE502004000989D1 (en) | 2006-08-31 |
| EP1595264A2 (en) | 2005-11-16 |
| US7349517B2 (en) | 2008-03-25 |
| US20060215800A1 (en) | 2006-09-28 |
| KR20050100692A (en) | 2005-10-19 |
| JP4607858B2 (en) | 2011-01-05 |
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